various fixes
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@@ -80,6 +80,46 @@ different absorber thickness are shown in \cref{tab:proton_cdc_hitrate}.
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\label{tab:proton_cdc_hitrate}
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\label{tab:proton_cdc_hitrate}
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\end{table}
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\end{table}
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%\begin{table}[htb]
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%\begin{center}
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%\begin{tabular}{S S S S S}
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%\toprule
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%{\textbf{Absorber}} &{\textbf{Inner wall}} & {\textbf{Total CFRP}}&
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%{\textbf{Proton hit rate}} & {\textbf{Proton hit rate}}\\
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%{\textbf{thickness}} &{\textbf{thickness}} & {\textbf{thickness}}&
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%{\textbf{Phase-I TDR}} & {\textbf{New estimation}}\\
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%{(\si{\mm})} & {(\si{\mm})} & {(\si{\mm})} & {(\si{\Hz})}& {(\si{\Hz})}\\
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%\midrule
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%1 &0.5&1.5 & 4E+3 & 2 \\
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%0.5 &0.5&1.0 & 11E+3& 126 \\
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%0 &0.5&0.5 & 30E+3& 1436 \\
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%\bottomrule
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%\end{tabular}
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%\end{center}
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%\caption{CDC proton hit rates at different configuration of proton absorber
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%and inner wall. The momentum spreads for \SI{0.5}{\mm} thick inner wall are
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%taken from \cref{tab:comet_absorber_impact}.}
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%\label{tab:proton_cdc_hitrate}
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%\end{table}
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%\begin{table}[htb]
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%\begin{center}
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%\begin{tabular}{S S S S S S}
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%\toprule
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%{\textbf{Absorber}} &{\textbf{Inner wall}} & {\textbf{Total CFRP}}& {\textbf{Proton}} & {\textbf{Momentum}} & {\textbf{Integrated charge}}\\
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%{\textbf{thickness}} &{\textbf{thickness}} & {\textbf{thickness}}& {\textbf{hit rate}} &{\textbf{spread $\Delta p$}} &{\textbf{300 days}}\\
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%{(\si{\mm})} & {(\si{\mm})} & {(\si{\mm})} & {(\si{\Hz})} & {(\si{\keV\per\cc)}} &{(mC/cm)}\\
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%\midrule
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%1 &0.5&1.5 & 2 & 195 & 25\\
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%0.5 &0.5&1.0 & 126 & 167 & 60\\
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%0 &0.5&0.5 & 1436 & 133 & 160\\
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%\bottomrule
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%\end{tabular}
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%\end{center}
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%\caption{CDC proton hit rates at different configuration of proton absorber
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%and inner wall. The momentum spreads for \SI{0.5}{\mm} thick inner wall are
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%taken from \cref{tab:comet_absorber_impact}.}
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%\end{table}
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At the baseline design of \SI{0.5}{\mm}, the hit rate is only \SI{126}{\Hz},
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At the baseline design of \SI{0.5}{\mm}, the hit rate is only \SI{126}{\Hz},
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much smaller than the current estimation at \SI{34}{\kHz}. Even without the
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much smaller than the current estimation at \SI{34}{\kHz}. Even without the
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absorber, proton hit rate remains low at \SI{1.4}{\kHz}.
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absorber, proton hit rate remains low at \SI{1.4}{\kHz}.
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Binary file not shown.
@@ -30,13 +30,13 @@ for the COMET experiment}
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\mainmatter
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\mainmatter
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%%%\input{chapters/chap1_intro}
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%%%\input{chapters/chap1_intro}
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%\input{chapters/chap2_mu_e_conv}
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\input{chapters/chap2_mu_e_conv}
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%\input{chapters/chap3_comet}
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\input{chapters/chap3_comet}
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%\input{chapters/chap4_alcap_phys}
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\input{chapters/chap4_alcap_phys}
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%\input{chapters/chap5_alcap_setup}
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\input{chapters/chap5_alcap_setup}
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\input{chapters/chap6_analysis}
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\input{chapters/chap6_analysis}
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\input{chapters/chap7_results}
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\input{chapters/chap7_results}
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%\input{chapters/chap8_conclusions}
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\input{chapters/chap8_conclusions}
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\begin{backmatter}
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\begin{backmatter}
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\input{chapters/backmatter}
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\input{chapters/backmatter}
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